1.2. Lecture 2

1.2.1. More results about the exponential map

For the next result about the exponential map it will be useful to know the following fact from linear algebra.

Lemma 1.2.1.

Let X∈GLn⁡(ℂ)X\in\operatorname{GL}_{n}(\mathbb{C}). Then XX is conjugate to a matrix of the form D⁢UDU where DD is diagonal, UU is upper triangular with ‘1’s on the diagonal and DD and UU commute.

Proof.

(nonexaminable) This follows from Jordan normal form. Here’s a direct proof. Firstly write ℂn\mathbb{C}^{n} as a direct sum of generalised eigenspaces for XX: if λ\lambda is an eigenvalue of XX then we can write the characteristic polynomial P⁢(T)=(T−λ)a⁢Q⁢(T)P(T)=(T-\lambda)^{a}Q(T) where Q⁢(T)Q(T) does not have λ\lambda as a root and a≥1a\geq 1 is an integer. Then the image of Q⁢(X)Q(X) on ℂn\mathbb{C}^{n} is the generalised eigenspace of λ\lambda. The kernel of Q⁢(X)Q(X) is preserved by XX and XX does not have an eigenvalue equal to λ\lambda since λ\lambda is not a root of Q⁢(X)Q(X), which must be the characteristic polynomial of XX acting on ker⁡Q⁢(X)\ker Q(X). Thus

im⁡Q⁢(X)∩ker⁡Q⁢(X)={0}\operatorname{im}Q(X)\cap\ker Q(X)=\{0\}

and by the rank-nullity theorem

ℂn=im⁡Q⁢(X)⊕ker⁡Q⁢(X)\mathbb{C}^{n}=\operatorname{im}Q(X)\oplus\ker Q(X)

is a decomposition of ℂn\mathbb{C}^{n} as a direct sum of the λ\lambda generalised eigenspace and a subspace preserved by XX. Repeating for each eigenvector gives the required decomposition of ℂn\mathbb{C}^{n}. This reduces the proof of the statement to the case where XX has only one eigenvalue λ\lambda. In this case, we can inductively choose a basis 𝐯1,…,𝐯n{\bf v}_{1},\ldots,{\bf v}_{n} of ℂn\mathbb{C}^{n} such that, for 1≤i≤n1\leq i\leq n, the image of 𝐯i{\bf v}_{i} in ℂ/⟨𝐯1,…,𝐯i−1⟩\mathbb{C}/\left\langle{\bf v}_{1},\ldots,{\bf v}_{i-1}\right\rangle is an eigenvector of XX with eigenvalue λ\lambda. With respect to this basis, XX is then diagonal with λ\lambda’s on the diagonal, and we get the required decomposition with D=λ⁢IdD=\lambda\operatorname{Id}. ∎

Lemma 1.2.2.

The exponential function exp:𝔤⁢𝔩n,ℂ→GLn⁡(ℂ)\exp:\mathfrak{gl}_{n,\mathbb{C}}\to\operatorname{GL}_{n}(\mathbb{C}) is surjective.

Proof.

First prove it for all DD and UU in GLn⁡(ℂ)\operatorname{GL}_{n}(\mathbb{C}) as in Lemma 1.2.1. The case of diagonal matrices is more straightforward (Problem 1.2.3(a)) whereas for UU you can use that the power series for log⁡(U)\log(U) in terms of powers of U−IdU-\operatorname{Id} is actually a polynomial (Problem 1.2.3(b)).

Now consider D⁢UDU. If D=exp⁡(d)D=\exp(d) and U=exp⁡(u)U=\exp(u) then

D⁢U=exp⁡(d)⁢exp⁡(u)=exp⁡(d+u)DU=\exp(d)\exp(u)=\exp(d+u)

because dd and uu commute (so long as you choose dd and uu carefully — Problem 1.2.3(c)).

By Lemma 1.2.1 we have that for any XX in GLn⁡(ℂ)\operatorname{GL}_{n}(\mathbb{C}) there exists a PP in GLn⁡(ℂ)\operatorname{GL}_{n}(\mathbb{C}) such that P−1⁢X⁢P=D⁢UP^{-1}XP=DU where DD and UU have the form stated in the Lemma. By Lemma 1.1.2(v) we have

X=P⁢D⁢U⁢P−1=P⁢exp⁡(d+u)⁢P−1=exp⁡(P⁢(d+u)⁢P−1)X=PDUP^{-1}=P\exp(d+u)P^{-1}=\exp(P(d+u)P^{-1})

and thus exp\exp is surjective. ∎

Remark 1.2.3.

The lemma is not true over ℝ\mathbb{R}; as we will see, the determinant of exp⁡(X)\exp(X) is positive for all real matrices XX.

Lemma 1.2.4.

We have

detexp⁡(X)=exp⁡tr⁡(X).\det\exp(X)=\exp\operatorname{tr}(X).
Proof.

By Lemma 1.2.1 we can conjugate so that XX is an upper triangular matrix with diagonal entries λ1,…,λn\lambda_{1},\ldots,\lambda_{n}, and then note that exp⁡(X)\exp(X) is also upper triangular with diagonal entries exp⁡(λ1),…,exp⁡(λn)\exp(\lambda_{1}),\ldots,\exp(\lambda_{n}).

Thus

detexp⁡(X)=∏i=1nexp⁡(λi)=exp⁡(∑i=1nλi)=exp⁡tr⁡(X).\det\exp(X)=\prod_{i=1}^{n}\exp(\lambda_{i})=\exp\left(\sum_{i=1}^{n}\lambda_{% i}\right)=\exp\operatorname{tr}(X).

∎

The next proposition will be useful when we discuss Lie algebras of linear Lie groups.

Proposition 1.2.5 (Lie product formula).

For X,Y∈𝔤⁢𝔩n,kX,Y\in\mathfrak{gl}_{n,k} we have

exp⁡(X+Y)=limk→∞(exp⁡(Xk)⁢exp⁡(Yk))k.\exp(X+Y)=\lim_{k\to\infty}\left(\exp\left(\frac{X}{k}\right)\exp\left(\frac{Y% }{k}\right)\right)^{k}.
Proof.

We have

(exp⁡(Xk)⁢exp⁡(Yk))k\displaystyle\left(\exp\left(\frac{X}{k}\right)\exp\left(\frac{Y}{k}\right)% \right)^{k} =((Id+Xk+O⁢(1k2))⁢(Id+Yk+O⁢(1k2)))k\displaystyle=\left(\left(\operatorname{Id}+\frac{X}{k}+O\left(\frac{1}{k^{2}}% \right)\right)\left(\operatorname{Id}+\frac{Y}{k}+O\left(\frac{1}{k^{2}}\right% )\right)\right)^{k}
=(Id+X+Yk+O⁢(1k2))k\displaystyle=\left(\operatorname{Id}+\frac{X+Y}{k}+O\left(\frac{1}{k^{2}}% \right)\right)^{k}
=Id+X+Y+O⁢(1k)\displaystyle=\operatorname{Id}+X+Y+O\left(\frac{1}{k}\right)
=exp⁡(X+Y+O⁢(1k)).\displaystyle=\exp\left(X+Y+O\left(\frac{1}{k}\right)\right).

Now take the limit as k→∞k\to\infty. ∎

1.2.2. One-parameter subgroups

Lemma 1.2.6.

The map from ℝ\mathbb{R} to GLn⁡(ℂ)\operatorname{GL}_{n}(\mathbb{C}) given by

t⟼exp⁡(t⁢X)t\longmapsto\exp(tX)

is a differentiable group homomorphism.

We have

dd⁢t⁢exp⁡(t⁢X)=X⁢exp⁡(t⁢X)=exp⁡(t⁢X)⁢X.\frac{d}{dt}\exp(tX)=X\exp(tX)=\exp(tX)X.

In particular,

dd⁢t⁢exp⁡(t⁢X)|t=0=X.\left.\frac{d}{dt}\exp(tX)\right|_{t=0}=X.
Proof.

The given map is a group homomorphism by Lemma 1.1.2(iv).

By definition,

exp⁡(t⁢X)=∑k=0∞Xkk!⁢tk.\exp(tX)=\sum_{k=0}^{\infty}\frac{X^{k}}{k!}t^{k}.

As this power series (and its termwise derivative) are uniformly convergent on any compact subset, we can compute its derivative by differentiating termwise, which gives

dd⁢t⁢exp⁡(t⁢X)=∑k=1∞Xk(k−1)!⁢tk−1=X⁢exp⁡(t⁢X).∎\frac{d}{dt}\exp(tX)=\sum_{k=1}^{\infty}\frac{X^{k}}{(k-1)!}t^{k-1}=X\exp(tX).\qed
Definition 1.2.7.

A one-parameter subgroup of GLn⁡(ℂ)\operatorname{GL}_{n}(\mathbb{C}) is a differentiable group homomorphism f:ℝ→GLn⁡(ℂ)f:\mathbb{R}\to\operatorname{GL}_{n}(\mathbb{C}). That is, a differentiable map such that

f⁢(s+t)=f⁢(s)⁢f⁢(t)f(s+t)=f(s)f(t)

for all s,t∈ℝs,t\in\mathbb{R}.

The infinitesimal generator of a one-parameter subgroup ff is the element f′⁢(0)∈𝔤⁢𝔩n,ℂf^{\prime}(0)\in\mathfrak{gl}_{n,\mathbb{C}}.

The convention used here is a slight abuse of notation, f⁢(ℝ)f(\mathbb{R}) is the subgroup of GLn⁡(ℂ)\operatorname{GL}_{n}(\mathbb{C}) referred to in the definition but as the map defines the subgroup we just refer to the map.

Remark 1.2.8.

For a one-parameter subgroup ff, it actually suffices to require that ff is continuous. Differentiability then comes for free.

Indeed, if ff is continuous, the integral ∫0af⁢(t)⁢𝑑t\int_{0}^{a}f(t)dt exists. Moreover,

f⁢(s)⁢∫0af⁢(t)⁢𝑑t=∫0af⁢(s+t)⁢𝑑t=∫ss+af⁢(t)⁢𝑑t.f(s)\int_{0}^{a}f(t)dt=\int_{0}^{a}f(s+t)dt=\int_{s}^{s+a}f(t)dt.

The RHS is differentiable with respect to ss by the fundamental theorem of algebra. Therefore, to prove that f⁢(s)f(s) is differentiable, we only need to show that there is an a>0a>0 such that ∫0af⁢(t)⁢𝑑t\int_{0}^{a}f(t)dt is an invertible matrix. Now consider the function

F⁢(a)=1a⁢∫0af⁢(t)⁢𝑑t.F(a)=\frac{1}{a}\int_{0}^{a}f(t)dt.

It is well-defined for a≠0a\neq 0 and lima→0F⁢(a)=Id\lim\limits_{a\to 0}F(a)=\operatorname{Id}. Hence, for 0<a≪10<a\ll 1, F⁢(a)F(a) is invertible, and therefore so is a⁢F⁢(a)=∫0af⁢(t)⁢𝑑taF(a)=\int_{0}^{a}f(t)dt.

The following is a very important property of one-parameter subgroups: that they all come from the exponential map.

Proposition 1.2.9.

Let f:ℝ→GLn⁡(ℂ)f:\mathbb{R}\to\operatorname{GL}_{n}(\mathbb{C}) be a one-parameter subgroup with infinitesimal generator XX.

Then

f⁢(t)=exp⁡(t⁢X)f(t)=\exp(tX)

for all t∈ℝt\in\mathbb{R}. That is, all one-parameter subgroups arise from the exponential function.

Proof.

From the definition of one-parameter subgroups, we have

f′⁢(t)=lims→0f⁢(s+t)−f⁢(t)s=f⁢(t)⁢lims→0f⁢(s)−f⁢(0)s=f⁢(t)⁢f′⁢(0)=f⁢(t)⁢X.f^{\prime}(t)=\lim_{s\to 0}\frac{f(s+t)-f(t)}{s}=f(t)\lim_{s\to 0}\frac{f(s)-f% (0)}{s}=f(t)f^{\prime}(0)=f(t)X.

Now consider the differential equation

f′⁢(t)=f⁢(t)⁢X.f^{\prime}(t)=f(t)X.

By Lemma 1.2.6 we have exp⁡(t⁢X)\exp(tX) is a solution with the initial condition that f⁢(0)=Idf(0)=\operatorname{Id}. To show it is a unique solution suppose that g⁢(t)g(t) is also a solution. Then

(g⁢(t)⁢exp⁡(−t⁢X))′=g′⁢(t)⁢exp⁡(−t⁢X)−g⁢(t)⁢exp⁡(−t⁢X)⁢X=g⁢(t)⁢(X⁢exp⁡(−t⁢X)−exp⁡(−t⁢X)⁢X)=0,\left(g(t)\exp(-tX)\right)^{\prime}=g^{\prime}(t)\exp(-tX)-g(t)\exp(-tX)X=g(t)% \left(X\exp(-tX)-\exp(-tX)X\right)=0,

and thus g⁢(t)⁢exp⁡(−t⁢X)=D∈GLn⁡(ℂ)g(t)\exp(-tX)=D\in\operatorname{GL}_{n}(\mathbb{C}). Applying the initial conditions we get D=IdD=\operatorname{Id} and g⁢(t)=exp⁡(t⁢X)g(t)=\exp(tX). ∎

Example 1.2.10.

The map ℝ→SO⁢(3)={g∈GL3⁡(ℝ)|g⁢gT=Id,detg=1}⊆GL3⁡(ℝ)\mathbb{R}\to\mathrm{SO}(3)=\{g\in\operatorname{GL}_{3}(\mathbb{R})\,|\,gg^{T}% =\operatorname{Id},\,\det g=1\}\subseteq\operatorname{GL}_{3}(\mathbb{R}) taking θ\theta to rotation by θ\theta about a fixed axis is a one-parameter subgroup. Problem 1.2.3 asks you to find its infinitesimal generator.

1.2.3. Exercises

.

Problem 3. Let 𝔫\mathfrak{n} be the ℂ\mathbb{C}-vector space of strictly upper triangular matrices (0’s on the diagonal) and let N={g∈GLn⁡(ℂ)|g=Id+X,X∈𝔫}N=\{g\in\operatorname{GL}_{n}(\mathbb{C})\,|\,g=\operatorname{Id}+X,X\in% \mathfrak{n}\}.

In this problem we will see that the restriction of the exponential to 𝔫\mathfrak{n} is a diffeomorphism onto NN.

  1. (a)
    ​

    Let X∈𝔫X\in\mathfrak{n}. Show that Xn=0X^{n}=0.

  2. (b)
    ​

    Show that exp⁡(X)∈N\exp(X)\in N for X∈𝔫X\in\mathfrak{n}.

  3. (c)
    ​

    Show that, for g∈Ng\in N, the logarithm log⁡(g)=∑k=1∞(−1)k+1⁢(g−I)kk\log(g)=\sum_{k=1}^{\infty}(-1)^{k+1}\tfrac{(g-I)^{k}}{k} is in fact a finite sum (and hence converges).

  4. (d)
    ​

    Show that exp|𝔫\exp|_{\mathfrak{n}} and log|N\log|_{N} are inverses of each other. Hint: this boils down to an identity of formal power series, which you can actually deduce from the corresponding fact over ℝ\mathbb{R}.

Problem 4. Using the previous question, fill in the gaps of the proof from the notes that

exp:𝔤⁢𝔩n,ℂ→GLn⁡(ℂ)\exp:\mathfrak{gl}_{n,\mathbb{C}}\rightarrow\operatorname{GL}_{n}(\mathbb{C})

is surjective.

  1. (a)
    ​

    Show all matrices of the form DD have a preimage.

  2. (b)
    ​

    Show all matrices of the form UU have a preimage.

  3. (c)
    ​

    Show all matrices of the form D⁢UDU have a preimage.

  4. (d)
    ​

    Is the exponential map exp:𝔰⁢𝔩2,ℂ→SL2⁡(ℂ)\exp:\mathfrak{sl}_{2,\mathbb{C}}\rightarrow\operatorname{SL}_{2}(\mathbb{C}) surjective? What about exp:𝔤⁢𝔩2,ℝ→GL2+⁡(ℝ)\exp:\mathfrak{gl}_{2,\mathbb{R}}\rightarrow\operatorname{GL}^{+}_{2}(\mathbb{% R})?

Problem 5. Let 𝐯∈ℝ3{\bf v}\in\mathbb{R}^{3} be a unit vector and let f:ℝ→S⁢O⁢(3)f:\mathbb{R}\to SO(3) be the map with f⁢(θ)f(\theta) being rotation by θ\theta about the axis 𝐯{\bf v} (the angle is measured anticlockwise as you look along the vector from the origin).

Show that ff is a one-parameter subgroup and find its infinitesimal generator in terms of 𝐯{\bf v}.